Step 1: Understanding the Question:
This question requires us to determine how the terminal settling velocity of a sphere depends on its diameter in the laminar settling regime.
This is a standard problem in particle mechanics and fluid-particle dynamics.
Step 2: Key Formula or Approach:
The particle Reynolds number is given as less than one (\( Re_p \lt 1 \)), which means the settling occurs in the Stokes' law (laminar) regime.
The formula for Stokes' terminal settling velocity (\( u_t \)) is:
\[ u_t = \frac{g \cdot d_p^2 \cdot (\rho_p - \rho_f)}{18 \cdot \mu} \]
where:
\( g \) is acceleration due to gravity,
\( d_p \) is particle diameter,
\( \rho_p \) is particle density,
\( \rho_f \) is fluid density,
\( \mu \) is fluid viscosity.
Step 3: Detailed Explanation:
• Identify the constant variables:
The density of both spheres is equal: \( \rho_{p1} = \rho_{p2} = \rho_p \).
They are falling through the same fluid, so \( \rho_f \) and \( \mu \) are identical for both.
Gravity \( g \) is constant.
• Establish the proportionality:
Since all other parameters are constant:
\[ u_t \propto d_p^2 \]
• Write the ratio for the two spheres:
Let subscript 1 represent the large sphere and subscript 2 represent the small sphere.
\[ \frac{u_{t1}}{u_{t2}} = \left(\frac{d_{p1}}{d_{p2}}\right)^2 \]
• We are given that the diameter of the large sphere is twice that of the small sphere:
\[ d_{p1} = 2 \cdot d_{p2} \quad \implies \quad \frac{d_{p1}}{d_{p2}} = 2 \]
• Substitute this ratio into the velocity relation:
\[ \frac{u_{t1}}{u_{t2}} = (2)^2 = 4 \]
Step 4: Final Answer:
The ratio of the terminal settling velocity of the large sphere to the small sphere is 4.